研究了含Kerr介质两模双光子Jaynes-Cummings模型腔场谱,给出了初始光场为光子数态、相干态和热光场时的计算结果,讨论了Kerr效应对谱结构的影响.发现一模腔场谱的频率可以被另一模初始场强灵敏地控制.
参考文献
| [1] | Agarwal G S. Vacuum-field Rabi oscillation of atoms in a cavity [J]. J. Opt. Soc. Am. B, 1985, 2(3): 480～485 |
| [2] | Eberly J H, Narozhny N B, Sanchez-Mondragon J J. Periodic spontaneous collapse and revival in a simple quantummodel [J]. Phys. Rev. lett., 1980, 44(20): 1323～1326 |
| [3] | Thompson R J, Rempe G, Kimble H J. Observation of normal-mode splitting for an atom in an optical cavity [J].Phys. Rev. Lett., 1992, 68(8): 1132～1135 |
| [4] | Rempe G, Walther H, Klein N. Observation of quantum collapse and revival in an one-atom maser [J]. Phys. Rev.Lett., 1987, 58(4): 353～356 |
| [5] | Jaynes E T, Cummings F W. Comparision of quantum and semiclassical radiation theories with application tobeam maser [J]. Proc. IEEE, 1963, 51(1): 89～109 |
| [6] | Buzek V, Jex I. Dynamics of two-level atom in a Kerr-like medium [J]. Opt. Comm., 1990, 78(5/6): 425～435 |
| [7] | Buzek V, Jex I. Emission spectra of two-level atom in a Kerr-like medium [J]. J. Mod. Opt., 1991, 38(5): 987～995 |
| [8] | 李高翔,彭金生.高Q Kerr介质腔中非简并双光子Jaynes-Cummings模型中光场的性质[J].物理学报,1993,42(9):1443～1451 |
| [9] | 冯健,宋同强,高云峰.高Q Kerr介质腔中非简并双光子Jaynes-Cummings模型中原子的辐射谱[J].光子学报,1996,25(11):976～981 |
| [10] | 高云峰,冯健,宋同强."两原子-双模腔场”系统的腔场谱[J].光学学报,2000,20(9):1194～1200 |
| [11] | 方卯发,刘惠恩.附加克尔介质Jaynes-Cummings模型的场熵演化[J].光学学报,1994,14(5):475～479 |
| [12] | Tahira Nasreen, Razmi M S K. Atomic emission and cavity field spectra for a two-photon Jaynes-Cummings modelin the presence of the Stark shift [J]. J. Opt. Soc. Am. B, 1993, 10(7), 1292～1300 |
| [13] | Ashraf M M. Cavity field spectra of the nondegenerate two-photon Jaynes-Cummings model [J]. Phys. Rev. A,1994, 50(6): 5116～5121 |
| [14] | 高云峰.冯健,宋同强.两原子双光子Jaynes-Cummings模型的腔场谱[J].物理学报,1999,48(9):1650～1658 |
| [15] | Eberly J H, Wodkiewicz K. Time-dependent spectrum of resonance fluorescence [J]. J. Opt. Soc. Am., 1977, 67(9):1252～1261 |
上一张
下一张
上一张
下一张
计量
- 下载量()
- 访问量()
文章评分
- 您的评分：
-
10%
-
20%
-
30%
-
40%
-
50%